日本地球惑星科学連合2018年大会

講演情報

[EE] Eveningポスター発表

セッション記号 S (固体地球科学) » S-CG 固体地球科学複合領域・一般

[S-CG56] アジア地域の地震・火山・テクトニクス

2018年5月20日(日) 17:15 〜 18:30 ポスター会場 (幕張メッセ国際展示場 7ホール)

コンビーナ:趙 大鵬(東北大学大学院理学研究科附属地震・噴火予知研究観測センター)、磯崎 行雄(東京大学大学院総合文化研究科広域科学専攻広域システム科学系)、Jianshe Lei(中国地震局地??力研究所)

[SCG56-P04] Particle Size Distribution of the active fault zone of Chelungpu fault and its implication for slipping and energetics of large earthquakes

*Wulan Okta Karunia1Li-Wei Kuo1Kuo-Fong Ma1Wen-Jie Wu1 (1.National Central University)

キーワード:Particle size distribution, Fractal dimension, Faulting mechanism, Fracture energy

The 1999 Mw7.6 Chi-Chi Earthquake occurred and produced ~10m slip along the northern Chelungpu fault in Taiwan. This study tries to estimate the fracture energy in past coseismic events and understands the plausible faulting mechanism within the active fault zone by obtaining the particle size distribution of fault gouge from the Taiwan Chelungpu-fault Drilling Project (TCDP). By means of Scanning Electron Microscope (SEM), Transmission Electron Microscope (TEM) and ImageJ analysis, we recognize the distinguished fracture and grain size within the 12-cm-black gouge and divide it into six layers. The particle diameter (D) and number of particles (N(D)), displaying as a log power-law distribution, mainly showed two values of fractal dimensions (FD) in the six layers. The first characteristic, including three layers, shows low FD values of ~2.7 and is characterized with big mineral grains and small total particle surface area, while the other shows high values of ~3.0 characterizing with aggregates down to dozens to hundreds of nanometer in size. Coincidentally, one layer of the high FD values has been recognized as the principal slip zone (PSZ) of the 1999 Mw7.6 Chi-Chi earthquake. It seems likely that the high FD layers may be experienced the similar processes during faulting, e.g., thermal pressurization. It is interesting that one high-FD-value layer displays identical textures to the PSZ showing a similar thickness, undeformed massive structure and a similar estimation of the fracture energy of 0.15 MJ/m2. Our evidence strongly implies that the large slip in the northern Chelungpu fault may be a consequence of the contribution of two PSZs. Finally, given the contribution of estimated fracture energy to the breakdown work which is 1.3%, the huge remaining part of breakdown work will be frictional heat which triggered several dynamic weakening processes such as thermal pressurization and melt lubrication.